A light emitting device comprises a waveguide having an electrically pumped gain region, a nonlinear medium, and an inclined mirror. Light pulses emitted from the gain region are reflected by the inclined mirror into the nonlinear medium in order to generate frequency-doubled light pulses. The gain region and the inclined mirror are implemented on the same substrate. The resulting structure is stable and compact, and allows on-wafer testing of produced emitters. The folded structure allows easy alignment of the nonlinear crystal.
Legal claims defining the scope of protection, as filed with the USPTO.
1. A light emitting device comprising: a waveguide having an electrically pumped gain region, a saturable absorber, a reflecting structure, a substrate, and a nonlinear medium, wherein said saturable absorber and said gain region are adapted to emit first light pulses from an end of said waveguide, said reflecting structure being adapted to reflect said first light pulses into said nonlinear medium, said nonlinear medium being adapted to generate second light pulses such that the optical frequency of said second light pulses is two times the optical frequency of said first light pulses; said gain region, said saturable absorber and said reflecting structure being implemented on said substrate such that said reflecting structure is adapted to change the direction of said first light pulses by an angle which is in the range of 70 to 110 degrees.
2. The device of claim 1 further comprising a partially reflecting structure to define an optical cavity together with a back reflector, said optical cavity comprising said gain region.
3. The device of claim 1 comprising a plurality of substantially parallel waveguides adapted to emit said first light pulses, the first light pulses emitted by said plurality of waveguides being coupled into a single nonlinear crystal.
4. The device of claim 1 wherein said first light pulses are adapted to pass through said common substrate.
5. The device of claim 1 further comprising a light-concentrating structure to collimate or focus light into said nonlinear crystal.
6. The device of claim 5 wherein said light-concentrating structure is a substantially cylindrical surface adapted to collimate or focus light in the direction of a fast axis of said first light pulses.
7. The device of claim 6 wherein said substrate has a cylindrical surface.
8. The device of claim 1 comprising a further waveguide to confine light of said first light pulses, said further waveguide comprising said nonlinear medium.
9. The light-emitting device of claim 8 wherein said waveguide comprises a tapered portion to concentrate light into a narrow part of said waveguide.
10. The device of claim 8 wherein said non-linear medium is a crystal having one or more convex facets to refract said first light pulses into said further waveguide.
11. The device of claim 1 wherein said reflecting structure has convex or concave form to change the divergence of said first light pulses.
12. The device of claim 1 wherein the first light pulses introduced into said nonlinear medium have a predetermined polarization, and said nonlinear medium has periodically poled zones to provide quasi phase matching such that said second light pulses are in the same phase for each poling period, the orientation of said zones being matched with polarization of said first light pulses.
13. The device of claim 12 further comprising a polarization-rotating element.
14. The device of claim 2 wherein said partially reflecting structure is a Bragg grating.
15. The device of claim 14 comprising a Bragg grating implemented on or in a nonlinear crystal to provide optical feedback through said nonlinear medium.
16. A method for generating light pulses by using a waveguide having an electrically pumped gain region, a saturable absorber, a reflecting structure, a substrate, and a nonlinear medium, said gain region, said saturable absorber and said reflecting structure being implemented on said substrate, said method comprising: providing first light pulses from an end of said waveguide by using said saturable absorber and said gain region, changing the direction of said first light pulses by an angle which is in the range of 70 to 110 degrees by said reflecting structure, and coupling said first light pulses into said nonlinear medium in order to generate second light pulses such that the optical frequency of said second light pulses is two times the optical frequency of said first light pulses.
17. The method of claim 16 further comprising changing the bias voltage of said saturable absorber between a first voltage level and a second voltage level.
18. A projecting device comprising: a light source, and projecting optics, said light source in turn comprising a waveguide having an electrically pumped gain region, a saturable absorber, a reflecting structure, a substrate, and a nonlinear medium, wherein said saturable absorber and said gain region are adapted to emit first light pulses from an end of said waveguide, said reflecting structure being adapted to reflect said first light pulses into said nonlinear medium, said nonlinear medium being adapted to generate second light pulses such that the optical frequency of said second light pulses is two times the optical frequency of said first light pulses; said gain region, said saturable absorber and said reflecting structure being implemented on said substrate such that said reflecting structure is adapted to change the direction of said first light pulses by an angle which is in the range of 70 to 110 degrees.
19. The projecting device of claim 18 comprising a two-dimensional modulator array.
20. The projecting device of claim 18 comprising at least one beam directing device, wherein said first light pulses are adapted to be generated by semi-passive Q-switching.
Cooperative Patent Classification codes for this invention. Click any code to explore related patents in that topic.
January 18, 2007
July 1, 2008
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